Current Switching With High Voltage Air Disconnect Or

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    Current Switching with High Voltage Air

    DisconnectorSalih Carsimamovic1, Zijad Bajramovic1, Miroslav Ljevak2, Meludin Veledar3, Nijaz Halilhodzic4

    Abstract. In the paper are presented results of switchingovervoltages investigations, produced by operations of air

    disconnector rated voltage 220 kV. Measurements of these

    switching overvoltages are performed in the air-insulated

    substation HPP Grabovica on River Neretva, which is an

    important object for operation of electric power system of Bosnia

    and Herzegovina. Investigations of operating of air disconnector

    type Centre-Break were performed in order to determine

    switching overvoltage levels that can lead to relay tripping in HPP

    Grabovica. During operations of disconnector (synchronization or

    disconnecting of generator from network) malfunctions of

    signalling devices and burning of supply units of protection relays

    were appeared. Also, results of computer simulations using

    EMTP-ATP [1] are presented.

    Key words: Switching overvoltages, air disconnector, air insulatedsubstations, secondary circuits.

    I. INTRODUCTION

    Switching operation in power stations and substations, high-

    voltage faults and lightning cause high levels of high

    frequency overvoltages that can be coupled with low voltage

    secondary circuits and electronic equipment unless they are

    suitably protected. The function of high-voltage air-break

    disconnectors is to provide electrical isolation of one part of

    the switchgear. Disconnector's standards define a negligible

    current interrupting capability (0.5 A) or a voltage between

    the contacts if it is not significantly changed. These values ofcurrents include the capacitive charging currents of bushing,

    bus bars, connectors, very short lengths of cables and the

    current of voltage instrument transformers. Disconnector's

    contacts in air-insulated substations (AIS) are moving slowly

    causing numerous strikes and restrikes between contacts.

    When the contacts are closed, the capacitive charging current

    flowing through the contacts ranges from 0.01710-3 to1.110-3 A/m for voltage levels 72.5 - 500 kV [2], dependingon the rated voltage and length of bus, which is switched.

    ______________________________________________

    This work was supported by the Ministry of Education and Science of the

    Canton Sarajevo.1

    Faculty of Electrical Engineering, University of Sarajevo, Zmaja od Bosnebb, 71000 Sarajevo, Bosnia and Herzegovina (e-mail: [email protected] ;

    [email protected])2 Energoinvest- Sarajevo, H.Cemerlica 2, 71000 Sarajevo, Bosnia and

    Herzegovina (e-mail: [email protected])3 ABB Representation for B&H, Zmaja od Bosne bb. TPC Sentada, 71000Sarajevo, Bosnia and Herzegovina (e-mail: [email protected])4 Public Enterprise Elektroprivreda BiH, HPP on Neretva, Jaroslava Cernija 1,

    88420 Jablanica, Bosnia and Herzegovina (e-mail: [email protected])_________________________________________________________

    Presented at the International Conference on Power Systems

    Transients (IPST05) in Montreal, Canada on June 19-23, 2005

    Paper No. IPST05 - 229

    Strikes and restrikes occur as soon as the dielectric strength ofthe air between contacts is exceeded by overvoltage.

    The distance between contacts, the contacts geometry and

    relative atmospheric condition defines the overvoltage at the

    instant of strike. Every strike causes high-frequency currents

    tending to equalize potentials at the contacts. When the current

    is interrupted, the voltages at the source side and the loading

    side will oscillate independently. The source side will follow

    the power frequency while the loading side will remain at the

    trapped voltage. As soon as the voltage between contacts

    exceeds the dielectric strength of the air, at that distance the

    restrike will occur, and so on.

    Successive strikes occurring during the closing and opening

    operations of the off-loaded bus by the disconnector are shownin Fig. 1 a and b, respectively.

    When closing takes place, the first strike will occur at the

    maximum value of the source voltage. Its values can be

    positive or negative. As the time passes a series of successive

    strikes will keep occurring at reduced amplitude, until the

    contacts touch. The highest transient overvoltage therefore

    occurs during the initial pre-arc, Fig.1 a.

    When the disconnector opening, restrikes occur because of the

    very small initial clearance between the contacts. At the

    transient beginning, the intervals between particular strikes are

    on the order of a millisecond, while just before the last strike;

    the period can reach about one half of cycle at power

    frequency, Fig. 1 b.

    a)

    b)

    Fig. 1. The voltage due to the disconnector switching

    a) Disconnector closing, b) Disconnector opening1-source side voltage, 2- load side voltage

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    During the switching time of operations of disconnectors at

    HPP Grabovica up to 500 restrikes were registered. In paper

    [3] there are up to 5000 restrike registered during switching

    operation of the disconnector. The maximum value of voltages

    and maximum value of the wave front increasing will take

    place at the maximum distance between contacts. For the

    purpose of the investigation of the insulation strength and

    induction of electromagnetic interferences (EMI), the most

    important are the first few strikes during the closing operation

    or the last few strikes during the opening operation. Each

    individual strike causes a travelling wave with the basic

    frequency on the order 0.5 MHz (330 kHz-600 kHz). Very fast

    transient overvoltage due to the closing operation of the

    disconnector at the load side of the test circuit is shown in Fig.

    2.

    Fig. 2. Very fast transient overvoltage due to the closing operation

    Channel 1- source side voltageChannel 2-load side voltage

    These high-frequency phenomena are coupled with the

    secondary circuits as a result of various mechanisms. The

    strongest interference is exerted by the stray capacities

    between the high-voltage conductors and the grounding

    system, followed by the metallic link between the grounding

    system and the secondary circuits. High-frequency transient

    current flowing in the grounding system generates potential

    differences, every time when a strike occurs between

    disconnector's contacts. In large secondary circuits, the

    potential differences are in the form of longitudinal voltages

    between the equipment inputs and the equipment enclosures.

    Depending on the type of secondary circuits used and the way

    they are laid, differential voltages may also occur. Such a

    coupling mechanism has a special effect on the secondary

    circuits of instrument transformers, and particularly on the

    connected instruments, since these circuits are always galvanic

    ally linked to the grounding system. Another factor, which

    cannot be discounted, is the linking of these circuits to theprimary plant via the internal capacities of the instrument

    transformers [4].

    Interference levels in secondary circuits of air-insulated

    substations during switching disconnectors depend on

    following parameters:

    -the transient voltages and currents generated by the switching

    operation;

    -the voltage level of the substation;

    -the relative position of the source of disturbances and

    susceptor;

    -The nature of the grounding network;

    -the cable type (shielded or unshielded);

    -the way the shields are grounded.

    There are two main modes of coupling secondary circuits with

    primary circuits [3, 5]:

    a) Electromagnetic or EM coupling, which can be split

    into three sub-categories; inductive, capacitive and

    radiative. The most important source of EM coupling

    is the propagating current and voltage waves on bus

    bars and power lines during high-voltage switching

    operations by disconnectors;

    b) Common impedance coupling, as a result of coupling

    caused by the sharing of a lumped impedance

    common to both the source and susceptor circuits.

    Common mode voltages, i.e., voltages measured between

    conductors and local ground, represent the main parameter

    used for assessing equipment immunity. The difficulty of

    comparing data comes from the fact that different authors

    performed measurements at different places (some

    measurements were made at the closest point to the

    disconnector being operated whereas others made

    measurements in the vicinity of the auxiliary equipment, i.e. in

    the relay room). Little information is available about thegrounding practice of the neutral conductor in CT or VT

    circuits, the quality and grounding of the sable shields as well

    as how the measurements have been performed. Therefore, the

    measured levels have to be analyzed very carefully before

    comparison and drawing any conclusions [5].

    Results of up to date measured common mode voltages at

    secondary circuits of CVT, CT and VT are presented in the

    paper [5]. There are maximum levels of the common mode

    voltages ranging from 100 Vpeak up to 2.5 kVpeak in the shields

    of the secondary circuits cables of the CT and VT. Results

    show that measured values of the common mode voltages at

    CT/CV secondary circuits, 220 kV ratings, range from

    Ucm=0.32 kVpeak [6] up to Ucm=0.85 kVpeak [7]. Resultsshown in paper [3] are for measured common mode voltages

    from 3-4 kV during switching operation by disconnector in 150

    kV switchgear up to 6-10 kV at 400 kV switchgear.

    II. RESULTS OF EXPERIMENTAL MEASUREMENTS ON

    SITE

    The last ten years of extensive analysis of disconnector and

    circuit breakers generated EMI measurements that have

    confirmed that disconnector operation with off-loaded busbar

    is the most important and typical source of interference in

    secondary circuits of substations. Measurements of switching

    overvoltages generated during disconnector operation in the

    air insulated substation HPP Grabovica on the river Neretva

    were performed. HPP Grabovica is an important object for

    operating of electric power system of Bosnia and

    Herzegovina. Investigations of operating of air disconnector

    type Centre-Break were performed in order to determine

    switching overvoltage levels that can lead to relay tripping in

    HPP Grabovica [8]. During operations of disconnector

    (synchronization or disconnecting of generator from network)

    malfunctions of signalling devices and burning of supply units

    of protection relays were appeared. Malfunctioning of

    auxiliary circuits were manifested by tripping relay of

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    differential protection of the generator, phase '4'- signalization

    on relay box 'ZB I' and signalling fire in 35 kV control panel.

    At the same time sparking between primary terminals of the

    current transformer (CT) was occurred. Malfunctioning of

    signalling circuits were lower (not eliminated) with installing

    shielded cables.

    Also, independent of switching operation of air insulated

    disconnectors, during synchronization of generator AG1 on

    network, its happened that one of the pole of 220 kV circuit

    breaker failures. In this case generator AG1 worked in motor

    regime. Because of that, HPP Grabovica plans to install circuit

    breakers on generators voltage (10,5 kV) [9].

    The field tests were performed at the test circuit at HPP

    Grabovica, Fig. 3.

    Fig. 3. The considered test circuit

    VT-voltage transformer (220/3/0.1/3/0.1/3 kV), CT-current transformer(200/1/1 A), CVD-capacitive voltage divider, CB-circuit breaker with two

    interrupting chambers and parallel capacitors (SF6 220 kV, 1600 A), Dc-

    disconnector (220 kV, 1250 A), MOSA-metal oxide surge arrester (Ur=199,5

    kV, 10 kA), PT-power transformer (64 MVA, 242/10,55% kV, YD5), AG1-generator 1 (64 MVA, 10,55% kV)

    The recorded wave shape of the overvoltage at the load side is

    shown in Fig. 4. The overvoltage factors at busbar, k, wererecorded up to 1.16 p.u. with the dominant frequency of

    considered transient fd equal to 0.536 MHz. Common mode

    voltages, Ucm, at VT were up to 708 Vpeak, with dominant

    frequency equal to 1.31 MHz.

    Fig. 4. Waveshape of the overvoltage

    Channel 1-voltage at CVD; ch 1 (2.5 V/div), probe 1x100, ratio 455

    Channel 2-voltages at secondary of VT; ch 2 (5 V/div), probe 1x100

    III. MODELING OF THE TEST CIRCUIT

    Computer simulations were performed on the model of test

    circuit containing elements drawn in Fig. 5. Overvoltages at

    busbars were calculated during disconnector closingoperations, for the same substation layout on which

    measurements were carried out.

    CB

    VT

    CVD

    arc

    PTstray

    connection

    wire

    connection

    tubeDc

    II

    IIII

    II

    busbars 220 kV

    model of

    network 220 kV

    CIIIIIII

    Ccb

    CT+MOSA

    C

    Fig. 5. Model of the test circuit

    Arc-4 ; stray-200 pF; connection tube Z=370 ; CVD-R=300 , C=1 nF;VT-500 pF; CB-2 capacitors, each C2 nF, (capacitance of open contacts,each C20 pF), Ccb=100 pF; CT-500 pF; MOSA-100 pF; connection wireZ=440 ; PT-3.5 nF

    The waveshape of simulated overvoltage surge at load side is

    given in Fig. 6. The difference between magnitudes of

    measured and simulated overvoltages is 5 %. The dominant

    frequency of simulated overvoltage is 0.620 MHz. Comparison

    between results of measured and calculated overvoltagescertified a good agreement of obtained values.

    245 kV4400 pF

    CVD

    Relay room

    AG1

    1

    MOSA

    M

    HPP GRABOVICA LAYOUT

    OL TO RP JABLANICA M

    M0.2 mH1250 A

    Dc

    VT

    CB

    CT

    PT

    BUS BARS 220kV 3~50 Hz, 1250 A

    1nF300

    0.44F

    2nF

    2nF

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    (f ile grabo-kontrola.pl4; x-var t) v :XX0007

    2.858 2.860 2.862 2.864 2.866 2.868 2.870 2.872[ms]-200

    -150

    -100

    -50

    0

    50

    100

    [kV]

    Fig. 6. Waveshape of simulated overvoltage surge

    When the Capacitive Voltage Divider (CVD) was excluded,

    there were higher values of calculated overvoltages (15%

    higher on amplitude and 6 % on frequency). Capacitive divider

    due to primary resistor equal to 300 and primary capacitanceequal to 1 nF influences on overvoltage at the same

    measurement point causing attenuation and damping oftransient overvoltrages.

    In order to reduce EMI in secondary circuits the best way is to

    reduce sources of interference emission during switching of air

    insulated disconnector. One of the ways of reducing is to

    install disconnecting circuit breakers. Substation disconnectors

    isolate circuit breakers from rest of the system during

    maintenance and repair. The maintenance requirements for

    modern SF6 high voltage circuit breakers are lower than

    maintenance demands made on disconnectors, which means

    one of reasons for disconnectors removed. Installing

    disconnecting circuit breaker there are no needs for switching

    operation of disconnectors. With disconnecting circuit

    breakers it is still possible to isolate the line, but lowmaintenance requirements means it is no longer necessary to

    isolate the circuit breaker. The disconnecting breaker had to be

    designed to safety lock in the open position, and to meet all

    voltage withstanding capabilities and safety requirements of

    disconnectors.

    Another way of reducing sources of interference emission is to

    install circuit breaker without parallel capacitors to contacts.

    This suggestion is based on analyses performed on three

    circuit models:

    a) model of CB with two breaking chambers and paralelcapacitors and VT on netvork side of CB;

    b) model of CB with two breaking chambers and withoutparalel capacitors and VT on netvork side of CB

    c) model of CB with two breaking chambers and withoutparalel capacitors and VT on generator side of CB

    Magnitudes of simulated overvoltages are presented in Table

    I. Voltages are measured in point of connection of VT, CT and

    PT.

    TABLE I

    MAGNITUDES OF SIMULATED OVERVOLTAGES

    Connection point

    Circuit model

    VT CT PT

    a) model of CB with

    two breaking chambersand paralel capacitors

    and VT on netvork side

    of CB

    169 kVf=620 kHz

    47 kVf=1,1 MHz

    51 kVf=620 kHz

    b) model of CB withtwo breaking chambers

    and without paralel

    capacitors and VT on

    netvork side of CB

    177 kV

    f=900 kHz

    560 V

    f=1,4 MHz

    165 V

    f=1,4 MHz

    c) model of CB with

    two breaking chambers

    and without paralel

    capacitors and VT on

    generator side of CB

    320 Vf=1,1 MHz

    320 Vf=1,1 MHz

    160 Vf=1,1 MHz

    Overvoltages on generator side of 220 kV CB during

    switching of disconnectors could be up to 320 V in the case of

    installing instrument voltage transformer (VT) on generator

    side of CB without parallel capacitors (near instrument current

    transformer CT). This case causes installing of circuit breakerat generators voltage (10,5 kV) for synchronization of

    generator to network (better conditions for synchronization).

    This solution of installing circuit breakers on generators

    voltage resulted from problems have occurred during

    synchronization of generatror with current 220 kV CB.

    IV. CONCLUSION

    Switching overvoltages due to disconnector operations have

    been analysed on the existing 220 kV AIS on HPP Grabovica.

    Measurements and calculations were conducted on the

    characteristic points in AIS, in order to determine the level of

    the EMI.

    The result of measurements has shown that high frequency

    voltages on busbars occur with amplitudes up to 1.16 p.u. (233

    kVpeak) and the dominant frequencies up to 0.6 MHz.

    The difference between magnitudes of measured and calculated

    overvoltages is 5 % and 15.6 % on frequency.

    Measured common mode voltages at secondary circuits were

    from 430 V up to 708 V.

    CVD influences on overvoltages at the same measurement

    point on busbars causing attenuation and damping of transient

    overvoltages.

    Comparison of the transient computer simulations with field

    measurements showed that calculations could be used for

    assessment of the transient overvoltages due to disconnector

    switching.In order to reduce EMI in secondary circuits, it is suggested to

    install switching modules and disconnecting circuit breakers

    [10] or to install circuit breakers without parallel capacitors to

    contacts.

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    V. REFERENCES

    [1]EMTP-ATP, European EMTP-ATP Users Group e.V.

    [2] D.F.Peelo, J.H.Sawada, B.R.Sunga, R.P.P.Smeets, J.G.Krone, L.Van Der

    Sluis, 'Current interruption with high voltage air-break disconnectors', CIGRE

    2004, paper A3-301[3] Guide on EMC in Power Plants and Substations, CIGRE WG 36.04, Dec.

    1997

    [4] H.Remde, H.Schwarz, 'Transient overvoltages in CT and VT secondary

    circuits in high-voltage substations',ABB Review 1/91[5] C.Imposimato, J.Hoeffelman, A.Eriksson, W.H.Siew, P.H.Pretorius,

    P.S.Wong, EMI Characterization of HVAC Substations-Updated Data and

    Influence on Immunity Assessment, CIGRE 2002, paper on behalf of

    CIGRE/CIRED WG 36/S2-04

    [6] R.M.Naumov, P.L.Vukelja, 'Experimental Investigations of Transient

    Overvoltages in Secondary Circuits of 400 and 220 kV High VoltageSubstations', CIGRE SC36 Symposium, Lausanne, paper 500-05, 1993

    [7] R.J.Gavazza, C.M.Wiggins, 'Reduction of Interference on Substation Low

    Voltage Wiring', IEEE Trans. On Power Delivery, Vol. 11, No.3, 1317-1329,July 1996

    [8] 'Overvoltages in primary and secondary circuits in HPP Grabovica due to

    disconnector switching', Faculty of Electrical Engineering, Report No.L1410010/04, Sarajevo, 2004

    [9]D.Braun, L.Widenhorn and J.Ischi, Impact of the Electrical Layout on the

    Availability of a Power Plant, 11-th CEPSI Conference, 21-25 October

    1996, Kuala Lumpur, Malaysia[10] C-E. Slver, H-E. Olovsson, W.Lord, P.Neorberg and J.Lundquist,

    Innovative substations with availability using switching modules and

    disconnecting circuit breakers, CIGRE 2000, paper 23-102